# mathematical structures deï¬ned by identities

TRANSCRIPT

Mathematical Structures Defined by Identities

Constantin M. Petridi,11 Apollonos Street, 151 24 Maroussi (Athens), Greece, Fax+30-1-6129250

In part - collaboration withPeter B, Krikelis, Mathematics Dep., Athens University,

e-mail [email protected]

Abstract

We propound the thesis that there is a ”limitation” to the number of possible struc-tures which are axiomatically endowed with identities involving operations. In the caseof algebras with a binary operation satisfying a formally irreducible (to be explained)identity between two n-iterates of the operation, it is established that the frequency ofsuch algebras goes to zero like e−n/16 as n →∞. This is proved by a suitable ordering andlabeling of the expressions (words) of the corresponding free algebra and the formationof a series of tableaux whose entries are the labels. The tableaux reveal surprising sym-metry properties, stated in terms of the Catalan numbers 1

n+1

(2nn

)and their partitions.

As a result of the defining identity and the tableaux all iterates of order higher than nfall into equivalence classes of semantically equal ones. Classnumbers depending on thetableaux are calculated for all algebras of order n = 3 (and partially for n = 4). Certainclassnumbers are invariants in the sense that for algebras of same order they are equal.Algebras with several operations of any arity are considered. A generalization of Catalannumbers depending on homomorphisms of the structure is proposed and correspondinggenerating functions set up. As an example of this, a kind of skein polynomials are con-structed characterizing the formal build-up of iterates. As no distinction is made betweenthe various algebras, isomorphic or not, which are models of the identity the results canalso be formulated in terms of varieties with signature the identity in question. 1

1. Introduction

1.1. Our basic thesis is that in the ocean of mathematical structures defined by identitiesthe essential ones, the ones which are liable to give rise to important developments, are few.Such an assertion may sound presumptuous. We believe, however, that our findings, exposedin this paper, constitute the first steps towards validating our claim.

Above statement necessitates of course to make clear the intuitive meaning of the wordsstructure, ocean, essential and few. We think that every mathematician, irrespective of hisspecial area of interest, has the same notion in mind of the word structure, codified in any ofthe various formulations which evolved in the course of time. Ocean refers to the multituderesulting from our freedom to imagine and write down formally any combinations of elementsand concepts entering in the definition of structure. Structures axiomatically endowed withidentities involving operations within the underlying universe are called, as usual algebras,resp. varieties for the totality of algebras of same signature. The meaning of few is harderto describe. But let us say it entails a kind of measure for a class of algebras having aspecific property in relation to the totality of pertinent possible algebras. The establishmentof such a specific property and of the relevant measure will become clear in the sequel at

1This remark was pointed out to me by Prof. Tom C. Brown, Simon Fraser University, Burnaby, B.C.,Canada.

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least for the algebras which will be considered. As to the term essential structure this isactually the great unknown and only conjectures can be made if one is to be honest. Toillustrate this characterization we would outright say that an algebra with a binary law V xysatisfying V V xyz = V xV yz is undeniably essential. This meager functional equation over aspecified universe (set) for its variables is simply astounding. It pervades the greater part ofmathematics, running like Ariadne’s thread through the labyrinth of mathematical theories,old and modern. The rich harvest of deep results which have been obtained thanks to itsvalidity - not to say anything, platonically speaking, of those which are still out there waitingto be unveiled - bears out the assertion. Is this only due to the fact that its basic models arethe natural numbers and their extensions, as well as the various groups? Or is there a muchdeeper reason that more complicated axiom systems involving identities, are rare among allpossible structures we can think of? Dieudonne, in another context, has voiced similar doubtsby saying in his introduction to the ”Abrege d’ histoire des Mathematiques 1700-1900” that”... l’ etude des algebres non - associatives les plus generales, n’ont guere justifie par desapplications a des problemes anciens les espoirs de leurs auteurs” .

Groups aside (associative identity), the importance of identities for breaking new groundin mathematics can hardly be emphasized enough. With the exception perhaps of parts ofpure geometry, it is a task indeed to seek out mathematical theories where identities are notpresent either in their axioms or in their developments. Just consider whether the theory ofLie groups and algebras would at all have been possible were it not for the Jacobi identity.Another case in point is the Burnside problem for groups with generators whose elementssatisfy the identity xn = 1. The celebrated Euler identity in eight variables, crucial in provingthat every positive integer is a sum of four squares, offers another example.

Our investigations have been motivated by our belief, corroborated by examination of loworder algebras, that there is a limitation restricting the number of novel algebras we canpostulate. Unless we are cunning and lucky to pick the right ones, the ones we propose tocall essential. The search for these and their classification is the main goal. Our paper, infour sections, is a first step in this direction. Section 2 deals with algebras whose binaryoperation V x1x2 satisfies an identity of order n, i.e. an equality between two n-iterates ofV , which cannot be formally reduced (to be explained) to an identity of lower order. It willbe shown that the number of such algebras is of the order of S2

ne−n/16 as n → ∞, whereSn = 1

n+1

(2nn

), the nth Catalan number. Since formally there are S2

n different n-identities,this of course means that the frequency of such algebras goes to zero as n → ∞. Theproof is by a novel method we introduce namely that of tableaux, which reveal unexpectedproperties yielding this result. Section 3 expounds the semantic consequences of the definingidentity. All iterates of order higher than n fall into equivalence classes of semanticallyequal ones (to be explained). For the associative identity equivalence classes of iterates ofsame order collapse into a single class. Depending on the tableaux used, all identities oforder n have the same classnumbers whose values are explicitly determined as functions ofcertain partitions of the Catalan numbers. If natural unicity constraints are imposed someessential algebras have been found. For example, for n = 3 the only essential algebras areV V V x1x2x3 x4 = V x1 V V x2x3x4 and V V x1V x2x3 x4 = V x1 V x2V x3x4, all others reducingto semigroups. Section 4 in form of notes and remarks, advances the idea that the methodof tableaux can be extended to any structure provided with an equivalence relation andgenerating formally new elements from elements already in the structure. Generalizations ofCatalan numbers depending on the homomorphisms of the structure, extension of the concept

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of homomorphism to several variables, skein polynomials associated to the iterates and otherallied material are included at the end. Annexed are Exhibits of tables used in the text.

2. Formal Part

2.1. Ordering of iterates of a binary operation. Construction of tableaux An andBn. The number of iterates of order n (n-iterates) of a binary operation V (x1x2) is the sameas the number of completely parenthesizing a product of n + 1 letters, with two factors ineach set of parentheses. As known, it is equal to the nth Catalan number Sn = 1

n+1

(2nn

).

We designate the n-iterates by Jn(xn . . . xn+1), i = 1, . . . , Sn, putting in evidence the n + 1variables x1, . . . , xn+1.

Suppose now we already have an ordering of the Sn−1 iterates V x1x2 of order n − 1. Writethem in a line in that order and, omitting indexes, form below table by substituting succes-sively each variable x by V xx:

Jn−11 (x1 . . . xn) Jn−1

2 (x1 . . . xn) · · · Jn−1Sn−1

(x1 . . . xn)——————— ——————– · · · ———————–

Jn−11 (V xx, x . . . x) Jn−1

2 (V xx, x . . . x) · · · Jn−1Sn−1

(V xx, x . . . x)Jn−1

1 (x, V xx . . . x) Jn−12 (x, V xx . . . x) · · · Jn−1

Sn−1(x, V xx . . . x)

· · · · · · · · · · · ·Jn−1

1 (x, x . . . V xx) Jn−12 (x, x . . . V xx) · · · Jn−1

Sn−1(x, x . . . V xx)

Above table comprises all Sn n-iterates Jni (x1 . . . xn+1), or Jn

i for short, i = 1, . . . , Sn, eachwith a certain multiplicity. Tableau An (see annexed Exhibit 1, for n = 4) is formed byassigning to each iterate a label number from 1 to Sn, starting with 1 for Jn−1

1 (V xx, x . . . xn)and going horizontally through all the lines of the table, from left to right, assigning the samelabel whenever the same iterate is encountered. We thus get a well-defined ordering of then-iterates, uniquely induced by the ordering of the (n− 1)-iterates.

n-Iterates can be generated from (n − 1)-iterates not just by inserting V xx in the variableplaces of (n− 1)-iterates, as done above, but also by forming

V (Jn−11 , x) V (Jn−1

2 , x) · · · V (Jn−1Sn−1

, x)V (x, Jn−1

1 ) V (x, Jn−12 ) · · · V (x, Jn−1

Sn−1).

Assigning to the iterates of this table the same labels as for An we obtain tableau Bn (seeExhibit 3).

Starting with tableaux A1 and B1 we can thus recursively form tableaux An and Bn, for any n.Tableau An has nSn−1 entries, tableau Bn has 2Sn−1 entries. Besides above two proceduresleading to An and Bn there is no other operation generating n-iterates from (n− 1)-iterates.There is a method based on arithmetical properties of An and Bn to write them out, butthis is quite involved so that at this stage we omit it. Labels have the advantage that it ismuch more convenient to peruse tables with numbers and find their properties, than tableswith expressions like V V xxV xV xx (see Exhibit 2). Whenever we refer to tableaux An andBn we shall indiscriminately use Jn

i or its label i(n, or just i, if n is fixed.

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2.2. Properties of tableaux An. Let Li, i = 1, . . . n be the n sets figuring respectively inthe lines of tableau An. If |M | denotes the cardinality of set M and M1∩M2 the intersectionof M1 and M2 then

|Li ∩ Lj | =

Sn−1 if i = j0 if |i− j| = 1Sn−2 otherwise

|Li ∩ Lj ∩ Lk| =

Sn−1 if i = j = k0 if at least one |i− j|, . . . , |j − k| is = 1Sn−3 otherwise

and generally for k = 1, 2, . . . , n

|Li1 ∩ Li2 ∩ . . . ∩ Lik | =

Sn−1 if i1 = i2 = . . . = ik0 if at least one |i1 − i2|, . . . , |ik−1 − ik| is = 1Sn−k otherwise

Sn are the Catalan numbers 1n+1

(2nn

).

Definition. The multiplicity M(Jni ), i = 1, ...Sn of an iterate Jn

i is the number of times itoccurs in tableau An.

The number of iterates with multiplicity k is

Tnk = 2n−2k+1

(n− 12k − 2

)Sk−1, k = 1, . . . ,

[n + 1

2

].

Above facts have been found by induction from low values of n, but we have no proofs. Maybesome competent combinatorialist can prove them.

Part of the tableau An, starting from the right, is a Young tableau, being a partition ofSn into n parts. The parts are the respective lengths in each line comprising sections ofconsecutive numbers of 1, 2, . . . , Sn. For example for n = 4 (Exhibit 3) we have by A4:

1 2 3 4 5 Sn = 14 = 5 + 5 + 3 + 16 7 8 9 10

11 12 1314

In the general case Sn = cn,1 + cn,2 + · · · + cn,n where the cn,j can be calculated recursivelyfrom following ”Pascal” triangle

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n\j 1 2 3 4 5 · · · n · · ·

1 1 S1 = 12 1 1 S2 = 1 + 1 = 23 2 2 1 S3 = 2 + 2 + 1 = 54 5 5 3 1 S4 = 5 + 5 + 3 + 1 = 145 14 14 9 4 1 S5 = 14 + 14 + 9 + 4 + 1 = 42· · · · · · · · · · · · · · · · · · · · · · · · · · · · · ·n cn,1 cn,2 · · · · · · · · · · · · cn,n Sn =

∑nj=1 cn,j

· · · · · · · · · · · · · · · · · · · · · · · · · · · · · ·

The recursion rule is

cn,j = cn−1,j−1 + cn−1,j + · · ·+ cn−1,n−1.

The numbers cn,j will be used in the semantic section of the paper. An extended ”Pascal”triangle up to n = 10 is appended (Exhibit 4). Out of curiosity we looked up the verticalsequences in Sloane’s Handbook of Integer Sequences and were surprised to see that e.g.1, 3, 9, 28, 90, 297, . . . are Laplace transforms coefficients; 1, 4, 14, 48, 165, 572, . . . are partitionsof a polygon by a number of parts. The numbers are known in the literature as ballot numbers,their values being cn,j = j

n

(2n−j−1

n−1

)(see Riordan, [1968], Aigner [2001]).

2.3. Formal reducibility of an identity and incidence matrix. An identity Jni = Jn

j

between two n-iterates is said to be of order n. It is formally reducible or simply reducible to anidentity of order n− 1 if V xx appears on both sides at the same variable place. For example,V V xV xx x = V x V V xx x of order 3 is actually formally reducible to V V xxx = V xV xxof order 2. Repeating the process, an identity of order n is reducible to an identity of lowerorder if there is an iterate Jk, k < n, appearing at the same variable place on both sidesof the identity. If there is no such Jk the identity is called formally irreducible, or simplyirreducible.

In order to calculate the number of reducible resp. irreducible identities we first form followingincidence matrix relative to tableau An of all possible S2

n identities of order n, includingJn

i = Jni and counting Jn

i = Jnj and Jn

j = Jni as different:

i\j Jn1 Jn

2 · · · JnSn

Jn1 · · · · · · · · · · · ·

Jn2 · · · · · · · · · · · ·· · · · · · · · · δ(Jn

i , Jnj ) · · ·

JnSn

· · · · · · · · · · · ·

where

δ(Jni , Jn

j ) ={

1 if Jni = Jn

j reducible0 if Jn

i = Jnj irreducible.

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The δ(Jni , Jn

j ) are determined by going successively through the lines of tableau An whoseconstruction is such that all identities between n-iterates on the same line are reducible toidentities of order n− 1 or lower. As an example we write out the incidence matrix relativeto tableau A3 for all possible 25 (S3 = 5) identities of order 3:

J31 J3

2 J33 J3

4 J35

∑j 1

J31 1 1 0 0 0 2

J32 1 1 0 0 1 3

J33 0 0 1 1 0 2

J34 0 0 1 1 0 2

J35 0 1 0 0 1 2

—I3 = 11

The incidence matrix of order n = 4 relative to tableau A4 is given in Exhibit 5, and is ofsize 14× 14 since S4 = 14.

The sumIn =

∑

i,j=1,...,Sn

δ(Jni , Jn

j )

gives the total number of reducible identities and therefore S2n−In is the number of irreducible

identities. For n = 3, I3 = 11 as shown above. One of the main goals is to calculate In.

2.4. Connection between multiplicity of Jni and

∑Snj=1 δ(Jn

i , Jnj ). The multiplicity

M(Jni ) of Jn

i was defined in subsection 2.1, as the number of times Jni occurs in tableau An.∑Sn

j=1 δ(Jni , Jn

j ) is the sum of 1’s in the i-th line of the incidence matrix. We shall provefollowing theorem which is fundamental in our calculation of In.

Theorem. Let M(Jni ) = k. Then

Sn∑

j=1

δ(Jni , Jn

j ) =k∑

ν=1

(−1)ν−1

(k

ν

)Sn−ν .

In other words∑Sn

j=1 δ(Jni , Jn

j ) does not depend on Jni but only on the multiplicity k of Jn

i .

Proof. Jni occurs in tableau An, k times, say once and only once on lines Lα1 , Lα2 , . . . , Lαk

,1 ≤ αν ≤ n, αν 6= αµ. Because of the construction of An it can never occur more than onceon the same line as all iterates of the line are formally different from each other. Applyingthe inclusion - exclusion principle we get

Sn∑

j=1

δ(Jni , Jn

i ) = |Lα1 |+ |Lα2 |+ · · ·+ |Lαk|−

|Lα1 ∩ Lα2 | − · · · − |Lαk−1∩ Lαk

|+

|Lα1 ∩ Lα2 ∩ Lα3 |+ · · ·+ |Lαk−2∩ Lαk−1

∩ Lαk|−

· · ·+ (−1)k−1|Lα1 ∩ Lα2 ∩ · · · ∩ Lαk|.

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The case of one of the |Lαν ∩ Lαµ | being 0 is impossible. This would mean according to 2.2that Jn

i occurs in tableau An in two consecutive lines. It can be proved however by inductionfrom An−1 to An that this cannot happen. In fact An is a ”Schachtelung” of Young tableauxdistanced vertically by at least 2 lines from each other as seen e.g. for An on annexed Exhibit3. As a consequence all |Lα1 ∩ Lα2 ∩ . . .| are also different from 0. Substituting their valuesas per 2.2 considering that αν 6= αµ we obtain

∑Snj=1 δ(Jn

i , Jnj ) =

∑kν=1(−1)ν−1

(kν

)Sn−ν as

required.¤

2.5. Calculation of In. We can now calculate In =∑Sn

i=1

∑Snj=1 δ(Jn

i , Jnj ). Since

∑Snj=1 δ(Jn

i , Jnj )

is the number of times Ji = Jj is reducible in the i-th line of the incidence matrix and, asindicated in 2.2, there are

Tn,k = 2n−2k+1

(n− 12k − 2

)Sk−1

(n− 12k − 2

)≥ 1

iterates Ji with multiplicity k we get for In:

In =[n+1

2]∑

k=1

Tn,k

Sn∑

j=1

δ(Jni , Jn

j )

.

The upper limit [n+12 ] for k is obtained from n − 1 ≥ 2k − 2, all Tn,k with k > [n+1

2 ] beingzero.

Inserting for∑Sn

j=1 δ(Jni , Jn

j ) its value found in 2.4 we get

In =[n+1

2]∑

k=1

Tn,k

[(k

1

)Sn−1 −

(k

2

)Sn−2 + · · ·+ (−1)k−1

(k

k

)Sn−k

]

and by changing the order of summation

In =

n+12∑

k=1

(−1)k−1Sn−k

[(k

k

)Tn,k +

(k + 1

k

)Tn,(k+1) + · · ·+

([n+1

2

]

k

)Tn,[n+1

2 ]

].

The evaluation of the brackets in this formula has transcended our efforts but straightforwardcalculations of In based on tableaux An for n = 3, 4, 5, 6, 7 and their respective incidencematrices have led us to surmise that

[n+12

]−k∑

ν=0

(k + ν

k

)Tn,k+ν =

(n− k + 1

k

)Sn−k.

For k = 1 this formula reduces to

1Tn,1 + 2Tn,2 + · · ·+[n + 1

2

]Tn,[n+1

2 ] = nSn−1,

which is certainly correct considering that tableau An has nSn−1 entries. Maybe applicationof the ”Snake Oil Method” or the ”Wilf-Zeilberger Method” which we have not tried willsucceed in proving this identity (see Wilf [1990]).

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Substituting the brackets in above formula by their values(n−k+1

k

)Sn−k and skipping the

upper limit [n+12 ] in the summation sign, as all

(n−k+1

k

)are zero for k > [n+1

2 ], the expressionfor In takes finally the form

In =∞∑

k=1

(−1)k−1

(n− k + 1

k

)S2

n−k.

2.6. Asymptotic evaluation of In. As there are S2n formally different algebras, counting

them as in section 2.3, defined by an identity Jni = Jn

j , and the number of reducible algebrasis In,

In

S2n

=∞∑

k=1

(−1)k−1

(n− k + 1

k

)(Sn−k

Sn

)2

is the probability (measure) for an algebra to be reducible and hence

1− In

S2n

is the probability that it be irreducible.

From the recurrence Sn = 22n−1n+1 Sn−1 for the Catalan numbers it can be easily shown by

induction from n to n + 1 that

Sn−k

Sn→ 1

4k for n →∞.

On the other hand(n−k+1

k

)is ∼ nk

k! for n →∞. The general term therefore of above seriesbehaves like

(−1)k−1 1k!

142k

nk.

Summing over k we can approximate In/S2n by

∞∑

k=1

(−1)k−1 1k!

( n

16

)k= 1− e−n/16,

and hence,

limn→∞

In

S2n

∼ limn→∞

(1− e−n/16

)= 1.

Above reasoning is of course not rigorous needing either a direct evaluation of the series or a”Fehlerabschatzung” of the difference with 1− e−n/16.

Stronger results can be obtained if instead of counting only the reducible identities of tableauAn we do also take into account the reducible identities of tableau Bn, which do not alreadyoccur in tableau An . For example from tableau B4 (Exhibit 3) we infer that J4

1 = J48

and J49 = J4

13 are formally reducible, a fact which can not be deduced from tableau A4. By”adding” tableau An and Bn to form An⊕Bn with (n+2)Sn−1 entries, we can again evaluate

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its corresponding incidence matrix which remarkably has the same properties as the incidencematrix of tableau An. The theorem that the sum of 1’s on a line of the incidence matrix is thesame for all Jn

i having the same multiplicity remains unchanged. The occurrence, however,of an iterate with multiplicity k has now been found to be

TAn⊕Bnn,k = Tn,k + 2 (Tn−1,k−1 − Tn−1,k) ,

with obvious notation. We have not pursued the calculations to find an expression for

IAn⊕Bnn =

[n+12 ]∑

k=1

TAn⊕Bnn,k

[(k

1

)Sn−1 −

(k

2

)Sn−2 + · · ·+ (−1)k−1

(k

k

)Sn−k

],

but evaluations up to n = 7 show as expected a much faster convergence of IAn⊕Bnn /S2

n to1, than that of In/S2

n.

2.7. Excursus on the implications of In/S2n → 1. The fact that IAn

n /S2n → 1 shows that

almost all n-identities reduce formally to identities of lower order. Since

S2n − In

S2n

∼ e−n/16

this means that there is almost no formally irreducible identity as n → ∞. This explicatesthe word few we used in the introduction regarding the possibility of stipulating structuresaxiomatically provided with an identity.

Formal irreducibility is an imperative requirement of an identity figuring in an axiom system:nobody would define a semigroup by V V V x1x2, x3, x4 = V V x1x2, V x3x4 (V x1x2 occurringin the same variable space on both sides) and not by V V x1x2, x3 = V x1, V x2x3 . If we asktherefore a mathematician to postulate an algebra with an identity of say order n = 35 andclaim it is a new structure, chances are high that his new product is redundant, as beingreducible to a lower order, maybe even to the associative law. If the question to turn out akilometer long identity is put to a computer, theoretically speaking, it is almost certain thatthe brainchild will be a hydrocephalus.

At this point we cannot resist the temptation to digress somehow from the mainstream ofour exposition. We have always wondered why mathematical axiom systems, theorems andformulas are so short, rarely taking more than a quarter page of a book to be formallyexpressed within a certain alphabet. Obviously, this is due to our anthropomorphic yardstickwhich is limiting our capacity to consider and manipulate long expressions. With the helpof computers the limits are just receding farther off. Unavoidably, however, this raises amajor question which, to our knowledge we haven’t seen addressed to before. Are theremathematical ”truths” which would require at least, say 100100100

pages of an ordinary bookto be expressed in some formal language, not including proofs? Clearly, abbreviations like∑

and formulations depending on a parameter n and increasing in length with increasingn cannot be considered to yield such statements if a specific large number is inserted for n.And of what nature and content would such monster theorems be which we wouldn’t be ableto read, let alone grasp?

But back to terra ferma and our smallish theorems until such a monster is discovered - ornot.

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3. Semantic Part

3.1. Classes of semantically equal iterates resulting from an identity. Semanticequality means that in an identity Jn

i (x1 . . . xn+1) = Jnj (x1 . . . xn+1) the two sides are formally

different but are the same (equal) for all xν running over the prescribed space for the variables.The usual properties of an equivalence relation hold.

The results of section 2 were mainly obtained by investigating the lines of tablaux An (oc-casionally also those of tablaux Bn). In the following, we will investigate the columns oftableaux An and Bn and derive semantic information regarding the iterates of V x1x2 oforder higher than n, as a consequence of the defining identity.

To illustrate the general case we will take an example drawn from tableaux A4 and B4

(Exhibit 3). Suppose we postulate a 3-algebra defined by the identity J32 = J3

4 or writ-ten out V (V xx, V xx) = V (x, V (V xx, x)). Using the enumerative labeling described in 2.1,(2(3, 4(3, 10(4, . . . stand respectively for J3

2 , J34 , J4

10, . . .) and going down columns 2 and 4 oftableaux A4 and B4 we deduce following identities:

From Tableau A4 From Tableau B4

2(3 = 4(3 2(3 = 4(3

——————— ———————2(4 = 4(4 3(4 = 8(4

7(4 = 9(4 10(4 = 13(4

4(4 = 12(4

5(4 = 10(4

This means that the 14 iterates of order 4 fall into 10 classes of semantically equal iterates iftableau A4 is used, namely (skipping upper indices):

{1}, {2, 4, 12}, {3}, {5, 10}, {6}, {7, 9}, {8}, {11}, {13}, {14}.

If B4 is also taken into account the number of classes is reduced to 8 because of the equivalenceproperties of semantic equality:

{1}, {2, 4, 12}, {3, 8}, {5, 10, 13}, {6}, {7, 9}, {11}, {14}.

We can now repeat the process by using either of above sets as defining identities and obtainvia tableaux A5 and B5 the equivalence classes of order 5 and their classnumbers (number ofclasses). This procedure, which can be continued indefinitely, splits the set of all iterates ofany order into equivalence classes of semantically equal ones, as a consequence of the initialdefining identity 2(3 = 4(3.

In the general case we start with an algebra postulated by an identity Jn = Jn between twoformally different iterates - several identities can also be considered as we shall see in section4. We can apply above procedure by using tableaux An+k and Bn+k, k ≥ 1, in a certainprescribed order, in which case the corresponding class sets and classnumbers will depend onthe chosen order. We shall restrict ourselves to using exclusively either tableaux An+k or bothtableaux An+k and Bn+k, in conjunction, which as said in 2.6 we denote by An+k⊕Bn+k. In

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the first case we have found a formula to calculate the classnumbers for any k, (see followingtheorem), without actually going through the laborious procedure of forming the successiveclass sets. This however is not giving the best results as shown by above example. Theactual minima of the classnumbers are obtained by using consistently tableaux An+k⊕Bn+k.We shall denote by hA

n+k, hBn+k and hA⊕B

n+k respectively the classnumbers in reference to thetableaux employed. As hA⊕B

n+k is the minimal number of the equivalence classes we shall omitthe indication A⊕B and simply call hn+k = hn+k(Jn = Jn) the classnumbers of the identity,for k ≥ 0. Below n the classnumbers are of course the Catalan numbers since the identity isof order n.

Writing Hn+ki , i = 1, ..., hn+k for the classes of order n+k we can list them as follows together

with their hn+k:

H01 h0 = 1

H11 h1 = 1

H21 H2

2 h2 = 2H3

1 H32 H3

3 H34 H3

5 h3 = 5· · · · · · · · · · · · · · · · · ·Hn−1

1 Hn−12 · · · · · · · · · Hn−1

Sn−1hn−1 = Sn−1

Hn1 Hn

2 · · · · · · · · · · · · HnSn−1 hn = Sn − 1

· · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · ·Hn+k

1 Hn+k2 · · · · · · · · · · · · · · · · · · Hn+k

hn+khn+k

· · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · ·

The main objective is to calculate the classnumbers hn+k for a given identity of order n andto classify the identities according to their classnumbers. A major find, conjectured, towardsthis aim, if we restrict ourselves to using only the sequence of the tableaux A1, A2, . . . , Ak, . . .is the

Theorem. All identities Jn = Jn of order n have the same classnumber hAn+k namely,

hAn+k(J

n = Jn) = Sn+k − cn+k+1,n+1 k ≥ 0

where the ci,,j are the numbers of the ”Pascal” triangle defined in 2.2.

Since hn+k < hAn+k, as any equivalence class from tableau A⊕B comprises all iterates of the

corresponding equivalence class of tableau A, we have

hn+k(Jn = Jn) < Sn+k − cn+k+1,n+1 k ≥ 0

which of course is stronger than the trivial hn+k < Sn+k, especially for big k.

Using tableaux Bn only it is easily seen that hBn+k = Sn+k − 2k, as all entries in the 2 lines

of Bn+k appear only once.

3.2. The algebra of classes. The classes Hpi can be taken as elements of a new algebra

with a binary composition law W (Hpi , Hq

j ) defined as follows:

Definition. If Jpi is a representative of the class Hp

i and Jqj is a representative of the class

Hqj then the class W (Hp

i ,Hqj ) is defined as the class of order p + q + 1 to which the iterate

V (Jpi , Jq

j ) of order p + q + 1 belongs.

11

The class W (Hpi ,Hq

j ) = Hp+q+1λ is uniquely defined as any other pair Jp

µ, Jqν , of representa-

tives will give an iterate V (Jpµ, Jq

ν ) semantically equal to V (Jpi , Jq

j ). The new law W (H1,H2)defined over the classes satisfies the same identity as the original algebra. It is a Lowenheim- Skolem denumerable model of the identity. The classnumbers hn+k now play the same roleas the Catalan numbers for the original algebra and corresponding tableaux can be formed.The process can be repeated giving a series of algebras.

3.3 Semantically reducible algebras. By semantic reducibility we mean that V (x, y) be-sides satisfying the defining formally irreducible identity, does also satisfy, because of inherentreasons of the structure, an identity of lower order. In the opposite case the identity is calledsemantically irreducible or essential.

So far the algebras considered were subjected to no constraint whatsoever besides the axiomof the defining identity. In the rest of this subsection we shall additionally provide that ifV (x, a) = V (y, a) then x = y and similarly V (a, x) = V (a, y) → x = y. These are naturalrestrictions and practically fulfilled in many structures of importance (unicity of solutions ofV (x, a) = b resp. V (a, x) = b in case they exist).

We have made a thorough investigation of all 3-algebras subject to above unicity propertyof V xy which led to the determination of all essential structures of that order as well as oftheir classnumbers.

The following theorem summarizes these results and the proof straightforward but tedious,clarifies the concept of semantic reducibility.

Theorem. There are only 2 algebras of order 3, semantically irreducible i.e.

V (V (V x1x2, x3), x4) = V (x1, V (V x2x3, x4)), (1(3 = 4(3)

andV (V (x1, V x2x3), x4) = V (x1, V (x2, V x3x4)), (3(3 = 5(3).

All other 3-algebras are reducible, formally or semantically to algebras of lower order, i.e. tosemigroups or to the free algebra of V xy with no identity. This theorem is true providedV (x, y) fulfills above unicity conditions.

Proof. We form the incidence matrix (see 2.3) 5× 5 of all 3-order identities resulting fromboth tableaux A3 and B3, i.e. from A3 ⊕ B3, in order to include also the reducible identitieswhich result from tableau B3 but not from tableau A3:

J1 J2 J3 J4 J5

J1 1 1 1 0 0J2 1 0 0 1J3 1 1 0J4 1 1J5 1

Because of symmetry only the upper triangle is considered.

We see that the only identities which are not formally reducible are the following five, indi-cated by 0’s in the matrix:

1(3 = 4(3, 1(3 = 5(3, 2(3 = 3(3, 2(3 = 4(3, 3(3 = 5(3.

12

Consider f.e. 1(3 = 5(3 and construct the equivalence classes of iterates of order 4 and 5, byapplying successively tableaux A4⊕B4 and A5⊕B5 as outlined in 3.1. From tableau A4⊕B4

we get successively (writing i(n or i for Jni ), by collection of classes having common elements,

following 6 identities which yield 8 (h4 = 8) equivalence classes for the 14 (S4 = 14) iteratesof order 4:

1(3 = 5(3

————1(4 = 5(4

6(4 = 10(4

3(4 = 13(4

2(4 = 14(4

1(4 = 11(4

9(4 = 14(4

{1,5,11}, (2,9,14}, {3,13}, {4}, {6,10}, {7}, {8}, {12}.

Repeating the same procedure with above classes we get from tableaux A5 ⊕B5 (Exhibit 3)-singletons can be omitted- following 14 classes for the 5-iterates (the equality sign betweenthe resulting 5-iterates has been omitted)

1(4 = 5(4 = 11(4 2(4 = 9(4 = 14(4 3(4 = 13(4 6(4 = 10(4

——————— ———————– ————– ————–1 5 11 2 9 14 3 13 6 10

15 19 25 16 23 28 17 27 20 246 10 34 7 32 37 8 36 29 333 13 38 4 26 41 11 40 17 272 14 30 5 24 42 7 37 16 281 11 29 3 22 38 6 34 15 25

23 28 39 24 36 42 26 41 32 37

{1, 5, 8, 11, 20, 24, 29, 33, 36, 40, 42}, {2, 9, 14, 30}, {3, 13, 22, 38}{4, 26, 41}, (6, 10, 34}, {7, 32, 37}, {12}, {15, 19, 25}, {16, 23, 28, 39}

{17, 27}, {18}, {21}, {31}, {35}

As we see one of the 14 5-order iterate classes is (1, 5, 8, 11, 20, 24, 29, 33, 36, 40, 42)which contains both 8(5and 11(5 as semantically equal. Let us write out in full the identity8(5 = 11(5 by substituting for the labels their corresponding 5-iterates (see Exhibit 2):

V (V (V x1x2, V (V x3x4, x5)), x6) = V (V (V x1x2, V (x3, V x4x5)), x6).

Because of the unicity assumption stipulated in the beginning of this section, we get succes-sively

V (V x1x2, V (V x3x4, x5)) = V (V x1x2, V (x3, V x4x5))

V (V x3x4, x5) = V (x3, V x4x5).

13

The last identity is of course the associative law so that the algebra 1(3 = 5(3 which is formallyirreducible, is actually a semigroup.¤The same can be shown to be true for the algebras 2(3 = 3(3 and 2(3 = 4(3, leaving as onlysemantically irreducible (essential!) algebras, the cases 1(3 = 4(3, 3(3 = 5(3, as stated inthe theorem. We would like to stress that above theorem is true at the present stage of theinvestigations as for the proof it suffices to form the equivalence classes of order up to 5. Butwho knows whether by proceeding to equivalence classes of orders 6, 7, . . ., n0, we won’t finda pair of n0 -iterates which would similarly also eliminate the cases 1(3 = 4(3, and 3(3 = 5(3?We have arithmetic evidence that this is rather unlikely.

It is possible to spare to trouble of writing out the iterates, which is extremely cumbersome,if we know beforehand which pairs of n-iterates automatically imply the semantic equality ofiterates of order 2, 3, ..., n− 1, respectively. This can be done with the help again of tableauAn. The number of such pairs can be shown to be

(n− k + 1)Sn−kSk(Sk − 1)

22 ≤ k ≤ n− 1.

Annexed here-with (Exhibit 6), by way of examples, are the tables of such iterates for n = 5,k = 2 (couples) and for n = 5, k = 3 (triples). They figure respectively in the two tableauxA5, connected by the sign l and should be read off vertically. Thus in tableaux A5, 8(5

and 11(5 figure in same column connected by l, implying associativity, as shown above. Forn = 5, k = 3 all pairs of 5-order iterates in same column connected by l, if semanticallyequal, automatically implicate the semantic equality of two 3-order iterates.

The rules of placement of the relational sign l, which we won’t expound, involve again theCatalan numbers and the numbers cnj of the ”Pascal” triangle defined in 2.2. This is furtherevidence of the wealth of information encoded in the tableaux An.

3.4. The series of classnumbers hn for identities of order 3 and 4. Equality in thissubsection means semantic equality.

As shown in 3.1 the partition of all N -iterates into hN classes of equal iterates induces as aresult of tableaux AN+1 ⊕BN+1 a partition of all (N + 1)-iterates into hN+1classes of equaliterates. The problem of one defining n-identity, is starting with hn = Sn − 1, to calculatethe series hn+1, ..., hn+k, ... . Generating functions

∑∞0 hntn can be defined and calculated in

some cases, for instance for 3(3 = 5(3.

We have carried out the investigation for all 3-identities and calculated the respective class-numbers up to n = 7, as well as the number of classes containing only 1 element (singletons).Beyond that the process gets unwieldy because of the fast growth of the Catalan numbers Sn.The following list summarizes our results for the 10 possible identities of order 3, obviouslyexcluding J

(3i = J

(3i and counting J

(3i = J

(3j and J

(3j = J

(3i as one identity. We have also

included the results for the formally reducible algebras because of the surprising fact that forsome of them the number of singletons are the Fibonacci numbers Fn:

14

Algebra Formally Classnumber Number ofreducible/ hn singletonsirreducible

———– ————– ——————– ————–1(3 = 2(3 reducible 2n−1 n ≥ 3 Fn n ≥ 31(3 = 3(3 reducible 2n−1 n ≥ 3 Fn n ≥ 31(3 = 4(3 irreducible 2n−1 n ≥ 3 n n ≥ 31(3 = 5(3 irreducible 4 n = 3 n n ≥ 3

8 n = 414 n = 520 n = 616 n = 7

2(3 = 3(3 irreducible 4 n = 3 n n ≥ 38 n = 414 n = 520 n = 624 n = 7

2(3 = 4(3 irreducible 4 n = 3 n n ≥ 38 n = 414 n = 520 n = 624 n = 7

2(3 = 5(3 reducible 2n−1 n ≥ 3 Fn n ≥ 33(3 = 4(3 reducible 2n−1 n ≥ 3 n n ≥ 33(3 = 5(3 irreducible 2n−1 n ≥ 3 n n ≥ 34(3 = 5(3 reducible 2n−1 n ≥ 3 Fn n ≥ 3

The behavior of 1(3 = 5(3 shows something which wouldn’t expect - repeated checks have notrevealed any error - namely that h7 = 16 is less than h6 = 20. Is this an indication that forall higher n the series h8, h9, . . . is bounded upwards? A phenomenon like that should not beexcluded. For example for the algebra defined by the two identities 1(3 = 4(3 and 3(3 = 5(3

the classnumbers are h3 = 3, h4 = 3 , hn = 1 for n ≥ 5. In final analysis the method oftableaux, as employed here, boils down to set theory. Namely substituting two sets M1,M2

of label numbers by the single set M1 ∪ M2 − M1 ∩ M2 provided M1 ∩ M2 is not empty.Surprises are to be expected!

For algebras of order 4 we have conducted some investigations to determine their classnumbersup to order 7. Since S4 = 14 there are 14×13

2 = 91 such identities, reducible and irreducible.We checked 10 of them, taken at random, and found that for 8 of them (f.ex. 11(4 = 14(4)the classnumbers seem to follow the rule

hn = Sn − 24n−3 − 1

3+

(n− 2)(n− 3)2

, 3 ≤ n ≤ 7.

As this expression becomes negative after n = 14 it certainly cannot give a general formulafor hn, unless strange phenomena appear for n > 14, similar to those observed for the algebra1(3 = 5(3. A computer search is imperative to decide the ambivalence.

15

4. Notes and Remarks

4.1. Algebras with several operations of any arity. The process of labeling iteratesand the construction of the relevant tableaux can be used for any algebra with any finitenumber of operations of any arity. The order n of an iterate is the number of operationsymbols figuring in each expression. The iterate (ai ≥ 0, pi ≥ 0):

J

{a1-V1 a2-V2 . . . ak-Vk

p1 p2 . . . pk

}

containing the a1-ry operation V1, p1 times, the a2-ry operation V2, p2 times, . . . has order

n = p1 + p2 + · · ·+ pk

and the number of variable places is

(a1 − 1)p1 + (a2 − 1)p2 + ... + (ak − 1)pk + 1.

It is possible to calculate the corresponding ”Catalan” numbers for the nunber of iterates viagenerating functions as done in the classical case k = 1, a1 = 2. Their generating functionφ(t) satisfies the equation

φ− 1t

= φa1 + φa2 + ... + φak

which reduces for k = 1, a1 = 2 to the classical equation φ−1t = φ2, giving the Catalan

numbers Sn, and similarly to the equations φ−1t = φa, for the higher ”Catalan” numbers:

San =

1(a− 1)n + 1

(an

n

), a ≥ 3.

The proof of above functional equation for the generating function is basically the same as inthe case of the ordinary Catalan numbers, but explicit formulas for the coefficients are onlypossible in exceptional cases (see Berndt [1965], p. 71).

We believe that the method of tableaux used in section 2 to calculate the number of reducibleidentities can be extended to the general case. Will the end result be the same, namely thatthe number of irreducible identities divided by the number of possible identities goes to zerowith increasing n ? We do not know. But if such is the case we are confronted again with alimitation in postulating new algebras of some order without risking to fall back, formally orsemantically, on lower order algebras already established as essential. A preliminary check inthe case of two binary operations V1x1x2 and V2x1x2 seems to confirm this contention.

4.2. Tableaux and Formal Languages. The method of tableaux we used to prove theresults of sections 2 and 3 is a special case of a general method applicable to formal languages.

Roughly described, it consists in assigning a ”length” n to the formulas (n-formulas) of thesystem and label them recursively from n to n + 1 in a specific order proper to the system.A formal deduction rule operating in the system generates (n+1)-formulas from n-formulas.This allows the recursive formation of tableaux by listing the labels of the n-formulas in a line,in increasing order, and beneath it the labels of the corresponding deducible (n+1)-formulas.

16

A (n + 1)-formula may be deducible from several n-formulas and thus have its label appearin several places of the tableau. The tableaux may be square, orthogonal, of unequal columnlengths, finite or infinite, depending on the system. An equivalence relation defined over theCartesian product of the set of n-formulas, subject to the rule that its validity extends to itsvalidity for the corresponding deducible (n + 1)-formulas, partitions all pairs of n-formulasinto two classes. One class will comprise the pairs which imply the validity of the equivalencefor at least one pair of (n − 1)-formulas. The other class will comprise the pairs which donot have this property. This introduces a concept of reducibility of a formal system equippedwith an equivalence relation, to a system of lower order. In the case of finite tableaux we canconsequently count the number of pairs in either class.

Above procedure applied to the formal language of expressions x, V xx, V V xxx, V xV xx,V V V xxxx, . . . generated by iterating the binary operation V xy yields the tableaux of ourpaper and leads to the asymptotic formula for the number of formally irreducible algebrasand the other results, the equivalence relation in question being the identity between two n-iterates of the operation.

4.3. Commutativity. In section 3 we have investigated n-iterates where the variable spacesare filled respectively by the same variable on both sides of the identity. But what happensif for example we have a structure (algebra) where following holds:

V (x1, V V x2x3, x4) = V (x3, V x2, V x4x1)

identically in all variables? The simplest case is of course commutativity V x1x2 = V x2x1.The general case is

Jn(x1, . . . , xn+1) = Jn(Pn(x1), . . . , Pn(xn+1))

where Pn is a permutation of the symmetric (n + 1)-group of the variables x1, x2 . . . , xn+1.The generation of (n + 1)-iterates from n-iterates is the same as in 2.1 but relabeling ofthe variables has to be made via following recursion in order to get the k-th line of thecorresponding tableau An+1:

Pn+1k (xν) =

Pn(xν) if 1 ≤ Pn(xν) ≤ kPn(xν+1) if k + 1 ≤ Pn(xν+1) ≤ nxk+1 if ν = n + 1

If Pn(xν) = xν we get the re-labeling of the variables used in 2.1.

As no single permutation can be excluded the total number of possible n -iterates is now(n + 1)!Sn and the relevant An tableau has n!Sn−1 lines and n columns.

Whether an asymptotic formula holds as in 2.6 is an open question of great interest in viewof the importance of commutativity and its higher analogues as well as other identities suchas the Jacobi identity with two operations.

4.4. Examples. Suppose a structure S formally defined as follows: If x ∈ S and y ∈ S thenAxy ∈ S where A is a fixed symbol. Putting V xy = Axy we get the basic system of iterateswith V replaced by A. If L(x) is the number of A’s figuring in x we obviously have

L(V xy) = L(x) + L(y) + 1

17

Setting both sides equal to n we get successively:

L(V xy) = L(x) + L(y) + 1 = n

∑

{z|L(z)=n}R [V xy = z] =

∑

κ+λ+1=n

R [L(x) = κ] R [L(y) = λ]

where R [E(x, y, ...) = a] denotes generally the number of solutions [xi, yi...] of any equationE(x, y, ...) = a with a fixed a. Since in the present case R [V xy = z] = 1 - an iterate J canbe formally expressed in only one way as V (J1, J2)- we get

∑

{z|L(z)=n}1 =

∑

κ+λ+1=n

R [L(x) = κ] R [L(y) = λ] ,

The left hand side being R [L(z) = n], i.e. the n−th Catalan number Sn, we get

Sn =∑

κ+λ+1=n

SκSλ

which is the classical recursion for these numbers.

Above reasoning and results can be widely generalized and in our view may be useful ininvestigating sequences over an alphabet generated by a law. Let us consider for examplea structure defined by a binary law V xy and an application L(x) onto the natural numberssubject to following homomorphism

L(V (xy) = P (L(x), L(y)),

where P (s, t) is a polynomial in s and t over the ring of integers satisfying a suitable positivitycondition. P need not be symmetric in x, y or have only positive coefficients. But e.g. let ustake P (s, t) = s2 + t2 + 2. A structure S obeying above homomorphism can be constructedas follows:

1. The elements x, y, . . . ∈ S are sequences of a’s and A’s.a is the generator, A a fixed symbol.

2. L(x) is the number of A’s figuring in x.3. If x ∈ S and y ∈ S, L(x) = s, L(y) = t, then

V (x, y) = Ax · · ·x︸ ︷︷ ︸stimes

Ay · · · y︸ ︷︷ ︸ttimes

∈ S

It is clear that L(V xy) = P (L(x), L(y)) = L(x)2 + L(y)2 + 2 as required.

Permutation of the A’s in the string of symbols x and y give rise to different structuressatisfying homomorphisms with the same polynomial law P (s, t). In the classical case V xy =Axy generates parenthesizing. But V xy = xAy does not.

4.5. ”Catalan” numbers relative to homomorphisms. The method used to obtainthe recursion formula for the Catalan numbers can be applied to the general case, providedevery element a of the structure can be uniquely expressed as V (x1x2). In other words theequation V (u, v) = a should have only one solution [x1, x2] : V (x1x2) = a.

18

Starting with a homomorphism L and a polynomial P , and proceeding as before we set

L(V xy) = P (L(x), L(y)) = n

and get the ”counting” equation∑

{z,|L(z)=n}R [V xy = z] =

∑

{s,t|P (s,t)=n}R [L(x) = s] R [L(y) = t]

where R[. . . = . . .] is the number of solutions of the equation in parenthesis and {. . . | . . .} theall - quantifier. Since we assumed that R[V xy = z] = 1 the left side reduces to

∑

{z|L(z)=n}1 = R[L(z) = n]

which we denote by SLn . We suggest to call these numbers the ”Catalan” numbers of the

structure relative to the homomorphism (L, P ). The recurrence relation now becomes

SLn =

∑

P (s,t)=n

SLs SL

t ,

where the summation extends over the solutions ≥ 0 of the Diophantine equation P (s, t) = n.If P (s, t) = s + t + 1 we get the ordinary Catalan numbers.

By way of generators a, b, · · · and fixed parameters (symbols) A,B, ... we may constructalgebras whose elements are words formed with the generators and the parameters. L(x)may count the number of A’s in x, or the number of B’s, or for that matter the number ofany configuration of A’s and B’s, such as for example AB. The composition law V xy can beset in such a way that given a polynomial P (s, t), the homomorphism L(V xy) = P (Lx,Ly)is fulfilled, as done in 4.4. In the general case R[V xy = z] for L(z) = n is a function of bothz and n not always equal to 1, depending on the underlying structure. Recursion formulasand generating functions, in the form of power or Dirichlet series for the ”Catalan” numbersSL

n = R[L(x) = n] are not always deducible, but in certain cases can be found. If e.g.P (s, t) = s + t + k and R[V xy = z] = n + l, with fixed integers k and l, and, assuming such astructure can be constructed as outlined, the counting equation leads to following differentialequation for the generating function G(t) =

∑SL

n tn

tG′(t) + lG(t)− tkG(t)2 =k−1∑

n=0

(n + l)SLn tn.

4.6. Sets of identities defining an algebra with a binary operation. Suppose ann-algebra is defined by classes hn of semantically equal n-iterates each class containing λi

different iterates and each of the Sn iterates figuring in one class only. Then

λ1 + λ2 + · · ·+ λhn = Sn.

Suppose further the operation V x1x2 satisfies the unicity condition for the solution V xa = band form the Sn−1 n-iterates V (Jn−1

1 , x), ..., V (Jn−1sn−1

, x). These iterates are semantically

19

different as otherwise there would be at least a pair Jn−1i = Jn−1

j and the algebra would beof lower order. Hence

hn ≥ Sn−1 =n + 24n + 2

Sn.

Substituting for Sn its above value we successively get

hn min(λi) ≤ λ1 + λ2 + ... + λhn ≤ 4n + 2n + 2

hn

min(λi) ≤ 4n + 2n + 2

< 4.

Therefore min(λi) ≤ 3, i.e. the set of classes defining the algebra must contain at least oneclass containing max. 3 iterates, if unicity conditions apply for the binary operation.

4.7. Multi-variable homomorphism. Homomorphisms L(x) are 1-variable functions. Wewere unable to find any reference in the literature to a generalization to more variables. Inour view a correct extension Ln(x1, . . . , xn) to several variables of this fundamental conceptwould be as follows:

Ln(V m(x1y1 . . . w1), . . . , (V m(xnyn . . . wn)) = Wm(Ln(x1x2 . . . xn), . . . , Ln(w1w2 . . . wn)),

where V m and Wm are m-ry operations, the upper indices indicating the number of variablesof the operations involved. This definition is purely formal, without regard to the domainsof validity of the operations, which have to be prescribed in a concrete application in orderto make it an identity.

For n = 1, m = 2 we get the usual homo (h)-morphism L(V xy) = W (Lx, Ly) for binarystructures. There is however a significant distinction between n = 1 and n ≥ 2, if V = W sothat all functions operate in the same domain. If n = 1 the series L(x), L(L(x)), ...Ln(x) =L(Ln−1(x)), ... i.e. the group of auto (a)-morphisms never leads outside the set of 1-variablea-morphisms. However, this is not true for n ≥ 2 where from the existence of one n-variablea-morphism we can deduce new a-morphisms of any order. If e.g. L(x1x2) is a 2-variablea-morphism then L(x2x2x3) = L(L(x1x2), x3) is a 3-variable a-morphism. The general resultestablishing the existence of a tower of a-morphisms is a consequence of the definition. Inthe case V = W the definition is reciprocal in the sense that if L is a n-variable a-morphismthen V is a m-variable a-morphism of L.

The search of h-morphisms resp. a-morphisms with many variables of a structure and theinvestigation of the corresponding groups by way of their composition (iteration) is of impor-tance as shown by the classical case in the Galois Theory of equations over a field. There areanalogous theorems if n ≥ 2, m ≥ 2:

1) Repeated application of the definition with V = W leads to the fact that L is also ana-morphism of any iterate J of V which in short we write L(J) = J(L).

2) In an equation between iterates of V , which may also involve constants a, b, c, l . . . ascoefficients, if r1, r2, . . . are roots of the equation then L(r1, r2, . . .) are roots of the sameequation whose corresponding coefficients are L(a, a, . . .), L(b, b, . . .) . . . .

3) If L(a, a, . . .) = a (idempotent) then L(r1, r2, . . .) is also a root of the same equation.

20

4) Considering the roots of an equation as functions of its coefficients it can be shown thatL is an a-morphism of these functions and vice-versa, if unicity conditions are fulfilled.

Above statements are only indicatively outlined but may convey an idea of what can be donewith multi-variable homomorphisms which of course are identities with several operations asdescribed in 4.1. We think they can prove useful for finite structures. We glimpse an eventualconnection with n-Categories (see Baez, Dolan, [1998]).

4.8. Relations between Catalan numbers. We give hereunder without proof somerelations for the classical Catalan numbers Sn = 1

n+1

(2nn

), n = 1, 2, ... which we haven’t seen

in the literature we are acquainted with:

1.∑

i1+···+iλ+1=n−λ

Si1Si2 . . . Siλ+1= Sn−

(λ + 1

1

)Sn−1+· · ·+(−1)k

(λ− k

k

)Sn−k

where k =[

λ2

], the greatest integer ≤ λ

2 and 1 ≤ λ ≤ n.

For λ = 1 this reduces to∑

i1+.i2=n−1 Si1Si2 = Sn.

2. Sn = cλ,1

∑

i1+i2=n−λ

Si1Si2+· · ·+cλ,λ

∑

i1+···+iλ+1=n−λ

Si1Si2 . . . Siλ+1

where cλ,i are the numbers of the ”Pascal” triangle defined in 2.2.

For λ = 1 this again reduces to the definition of the Catalan numbers.

3. limn→∞

1Sn

∑

i1+···+iλ+1=n−λ

Si1Si2 . . . Siλ+1=

λ + 12λ

, λ ≥ 1.

4. An iterate of V xx of order n is a string of 2n + 1 symbols each of which

is either a V or an x. It can therefore be written as

a1b1 · · · akbk with integers ai, bi ≥ 1,

thus uniquely assigning an integer 1 ≤ k < n to each iterate.

For example J(511 = V V V xxV xV xxx can be written as a1b1a2b2a3b3 = 321113

with k = 3.

An expression a1b1 . . . akbk represents an n-iterate of a binary operation,

is well formed so to say, iff k and the ai, bi satisfy one of following conditions:

i) k = 1, a1 = n, b1 = n + 1

21

ii) k ≥ 2, a1 + a2 + · · ·+ ak = n

b1 + b2 + · · ·+ bk = n + 1

a1 ≥ b1

a1 + a2 ≥ b1 + b2

..............................

a1 + a2 + · · ·+ ak−1 ≥ b1 + b2 + · · ·+ bk−1

Hence Sn − 1 is the number of integer solutions ≥ 1 of above Diophantine system,

which simultaneously gives an algorithm to decide in k steps whether any word

in V ’s and x’s is an n-iterate of the binary operation V xx the number of which

is Sn whose order is ∼ 1√πn−3/222n.

4.9. Skein polynomials of iterates of a binary operation. The build-up of an iterateJ can be characterized by a polynomial P (J ; a, b) of 2 variables in the following way. E.g.let us take again J

(511 and put indexes in the V ’s and x’s

V1V2V3x1x2 V4x3V5x4x5 x6.

The relation of a variable to the operations is not always the same. For example, x2 is withinthe ”Wirkungsbereich” (WB) of V1, V2 and V3 but outside of that of V4 and V5. Similarly x6

is within V1 but outside of V2, V3, V4, V5. This can easily been seen if the parentheses are putin place. A further distinction to be made is whether the variable is in the first place or thesecond place of an operation. In above example x3 is in the first place of V1, in the secondplace of V2 and in the first place of V4.

We substantiate these remarks by associating to each variable a monomial asbt with a, b ina commutative ring R. We could also assign monomials asbtck, c standing for being outsideof the WB but this doesn’t make any essential difference. The exponents s and t are thenumbers of the first resp. second place occurrences of the variable. We then sum thesemonomials to form a polynomial corresponding to the iterate in question. Setting 1 for thepolynomial of x we get by this procedure following table for the iterates Jn

i up to n = 3,listed in the ordering defined in 2.1 (Exhibit 2):

22

Iterate J Polynomial P (J)———— ———————x 1

V xx a + b

V V xxx a2 + ab + bV xV xx a + ab + b2

V V V xxxx a3 + a2b + ab + bV V xxV xx a2 + 2ab + b2

V V xV xxx a2 + a2b + ab2 + bV xV V xxx a + a2b + ab2 + b2

V xV xV xx a + ab + ab2 + b3

· · · · · ·

It is easily seen that the formation rule of P (J) obeys the homomorphism

P (V (J, J ′)) = aP (J) + bP (J ′).

If therefore R is the ring of integers the arguments of 4.3 can be applied verbatim. WritingP (Jn

i ; a, b) for the polynomial of Jni we have P (Jn

i ; 1, 1) = n + 1 and P (Jni ; a, b) = 1 if

a + b = 1. Because of this, simpler polynomials Q(J) can be defined by setting

Q(Jni ; a, b) =

P (Jni ; a, b)− 1

a + b− 1

withQ(V (J, J

′)) = aQ(J) + bQ(J

′) + 1

The functionGP (t) =

∑

J

tP (J) = t1 + ta+b + ta2+ab+b + ta+ab+b2 + · · ·

satisfies the functional equation

GP (ta)GP (tb) = GP (t)− t.

The functionGQ(t) =

∑

J

tQ(J) = 1 + t + ta+1 + tb+1 + · · ·

satisfies the functional equation

tGQ(ta)GQ(tb) = GQ(t)− 1,

which reduces to the Catalan equation for a = b = 1.

Collecting terms in GP (t) for which P (J) = P (J′) we may write

GP (t) =∑

J

NP tP (J)

23

where NP is the number of solutions J for which P (J) = Pi , where Pi is a specific polynomialof the series P1, P2, · · · listed above. The NP satisfy the equation:

NP =∑

{κ,λ | aPκ+bPλ=P}NPκNPλ

.

It was originally thought that there was a (1, 1) correspondence between the J ’s and theirpolynomials P (J) and our efforts to find the essential algebras Jn

i = Jnj consisted in equating

the corresponding polynomials P (Jni ; a, b) = P (Jn

j ; a, b) and look for distinctive propertiesof the resulting algebraic manifolds. The correspondence however is not (1, 1) which wouldmean that all Ni = 1. Already for n = 4,

P (J44 ) = P (J4

7 ) = a2 + ab + a2b + ab2 + b2 (= P ′)

so that NP ′ = 2.

Our attention has been drawn to the fact that the polynomials we constructed to reflect theway the iterates of a binary operation are built, bear a similarity with the polynomials ofknot theory.

4.10. Which algebras are essential? A conjecture. The theorem of 3.2 says that theonly essential algebras of order 3, subject to unicity conditions, are the following two:

V (V (V x1x2, x3), x4) = V (x1, V (V x2x3, x4)) (1(3 = 4(3)

V (V (x1, V x2x3), x4) = V (x1, V (x2, V x3x4)) (3(3 = 5(3).

We notice that as to their form these can be written respectively as

V (A, x) = V (x,A)

V (B, x) = V (x,B),

where A and B are the two iterates of order 2, J21 and J2

2 . On the other hand it is seen thatthe pairs (1, 4) and (3, 5) are the columns of tableau B3. Is this a lead sign that even in thegeneral case the essential algebras are given by the columns of tableaux Bn ? So that forn = 4 the essential algebras would be J4

1 = J49 , J4

3 = J410, J4

6 = J412, J4

8 = J413, J4

11 = J414,

and for any n they are given by the Sn−1 pairs

V (Jn−1i , x ) = V (x, Jn−1

i ) i = 1, ...Sn−1.

We suspect this to be true. Use of computer should help at least for low n’s.

24

References.

1. Aigner, M. [2001]: Catalan and other numbers: a recurrent theme, in AlgebraicCombinatorics and Computer Science, Eds. H. Crapo, D. Senato,Springer Verlag Italia, Milano

2. Baez, J., Dolan, J., [1998]: Higher - dimensional algebra III: n-Categories and thealgebra of opetopes, Adv. Math. 135 (1998), 145-206

3. Bakhturin Yu. R., Ol’shanskij A. Yu. [1991]:Identities, Encyclopaedia of MathematicalSciences Vol 18, Algebra II, Springer - Verlag, Berlin Heidleberg

4. Berndt, B. C. [1985]: Ramanujan’s Notebooks, Part I, Springer - Verlag, New York

5. Cohn, P. M., [1965]: Umiversal Algebra, Harper&Row, Ltd., London

6. Riordan, J. [1968]: Combinatorial Identities, J, Wiley, New York

7. Tarski, A. [1968]: Equational Logic and Equational Theories of Algebras, inContributions to Mathematical Logic, Studies in Logic and the Foundations ofMathematics, North - Holland Publishing Co., Amsterdam

8. Wilf, H. [1990]. Generatingfunctionology, Academic Press, Inc., San Diego

25

Exhibit 1

Ordering and labels of 4-iterates generated from ordering of 3-iterates.

1 V V V xxxx 2 V V xxV xx 3 V V xV xxx 4 V xV V xxx 5 V xV xV xx——————– ——————– ——————– ——————– ——————–

1 V V V V xxxxx 2 V V V xxxV xx 3 V V V xxV xxx 4 V V xxV V xxx 5 V V xxV xV xx6 V V V xV xxxx 7 V V xV xxV xx 8 V V xV V xxxx 9 V xV V V xxxx 10 V xV V xxV xx3 V V V xxV xxx 4 V V xxV V xxx 11 V V xV xV xxx 12 V xV V xV xxx 13 V xV xV V xxx2 V V V xxxV xx 5 V V xxV xV xx 7 V V xV xxV xx 10 V xV V xxV xx 14 V xV xV xV xx

1 V V V V xxxxx 3 V V V xxV xxx 6 V V V xV xxxx 8 V V xV V xxxx 11 V V xV xV xxx9 V xV V V xxxx 10 V xV V xxV xx 12 V xV V xV xxxx 13 V xV xV V xxx 14 V xV xV xV xx

Tableau A4

—————1 2 3 4 56 7 8 9 103 4 11 12 132 5 7 10 14

Tableau B4

—————1 3 6 8 119 10 12 13 14

26

Exhibit 2

Iterates Jni (n ≤ 4) Labels i(n

J01 x 1(0

J11 V xx 1(1

J21 V V xxx 1(2

J22 V xV xx 2(2

J31 V V V xxxx 1(3

J32 V V xxV xx 2(3

J33 V V xV xxx 3(3

J34 V xV V xxx 4(3

J35 V xV xV xx 5(3

J41 V V V V xxxxx 1(4

J42 V V V xxxV xx 2(4

J43 V V V xxV xxx 3(4

J44 V V xxV V xxx 4(4

J45 V V xxV xV xx 5(4

J46 V V V xV xxxx 6(4

J47 V V xV xxV xx 7(4

J48 V V xV V xxxx 8(4

J49 V xV V V xxxx 9(4

J410 V xV V xxV xx 10(4

J411 V V xV xV xxx 11(4

J412 V xV V xV xxx 12(4

J413 V xV xV V xxx 13(4

J414 V xV xV xV xx 14(4

J51 V V V V V xxxxxx 1(5

J52 V V V V xxxxV xx 2(5

. . . . . . . . .

J58 V V V xxV V xxxx 8(5

. . . . . . . . .

J511 V V V xxV xV xxx 11(5

. . . . . . . . .

J542 V xV xV xV xV xx 42(5

. . . . . . . . .

27

Exhibit 3

Tableaux An and Bn (n ≤ 5)——————————————–

A1 A2 A3 A4

1 1 1 2 1 2 3 4 52 3 4 6 7 8 9 10

B1 2 5 3 4 11 12 131 B2 2 5 7 10 14

1 B3

2 1 3 B4

4 5 1 3 6 8 119 10 12 13 14

A5

1 2 3 4 5 6 7 8 9 10 11 12 13 1415 16 17 18 19 20 21 22 23 24 25 26 27 286 7 8 9 10 29 30 31 32 33 34 35 36 373 4 11 12 13 17 18 25 26 27 38 39 40 412 5 7 10 14 16 19 21 24 28 30 33 37 42

B5

1 3 6 8 11 15 17 20 22 25 29 31 34 3823 24 26 27 28 32 33 35 36 37 39 40 41 42

Tableaux An ⊕Bn (n ≤ 5)—————————————

A1 ⊕B1 A2 ⊕B2 A3 ⊕B3 A4 ⊕B4

1 1 1 2 1 2 3 4 51 2 3 4 6 7 8 9 10

1 2 5 3 4 11 12 132 1 3 2 5 7 10 14

4 5 1 3 6 8 119 10 12 13 14

A5 ⊕B5

1 2 3 4 5 6 7 8 9 10 11 12 13 1415 16 17 18 19 20 21 22 23 24 25 26 27 286 7 8 9 10 29 30 31 32 33 34 35 36 373 4 11 12 13 17 18 25 26 27 38 39 40 412 5 7 10 14 16 19 21 24 28 30 33 37 421 3 6 8 11 15 17 20 22 25 29 31 34 3823 24 26 27 28 32 33 35 36 37 39 40 41 42

28

Exhibit 4

”Pascal” triangle for the numbers cn,j

n\j 1 2 3 4 5 6 7 8 9 10 . . .

1 1

2 1 1

3 2 2 1

4 5 5 3 1

5 14 14 9 4 1

6 42 42 28 14 5 1

7 132 132 90 48 20 6 1

8 429 429 297 165 75 27 7 1

9 1430 1430 1001 572 275 110 35 8 1

10 4862 4862 3432 2002 1001 429 154 44 9 1

· · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · · ·

cn,j = cn−1,j−1 + cn−1,j + cn−1,j+1 + · · ·+ cn−1,n−1

n∑

j=1

cn,,j = Sn

29

Exhibit 5

Incidence matrix for n = 4 relative to tableau A4 for all possible

S24 (= 142) identities J

(4i = J

(4j and calculation of I4

(J (4i denoted by i. Blank spaces denote 0’s )

δij ={

1 if identity reducible0 if identity irreducible

M(i) = Multiplicity of Ji

i\j 1 2 3 4 5 6 7 8 9 10 11 12 13 14∑

i 1 M(i)

1 1 1 1 1 1 5 12 1 1 1 1 1 1 1 1 8 23 1 1 1 1 1 1 1 1 8 24 1 1 1 1 1 1 1 1 8 25 1 1 1 1 1 1 1 1 8 26 1 1 1 1 1 5 17 1 1 1 1 1 1 1 1 8 28 1 1 1 1 1 5 19 1 1 1 1 1 5 110 1 1 1 1 1 1 1 1 8 211 1 1 1 1 1 5 112 1 1 1 1 1 5 113 1 1 1 1 1 5 114 1 1 1 1 1 5 1

——I4 = 88

Number of Jni with multiplicity k : Tn,k = 2n−2k+1

(n−12k−2

)Sk−1

For n = 4, k = 1 : T4,1 = 8

For n = 4, k = 2 : T4,2 = 6

In =[n+1

2 ]∑

k=1

(−1)k−1

(n− k + 1

k

)S2

n−k

I4 =2∑

k=1

(−1)k−1

(5− k

k

)S2

4−k =(

41

)S2

3 −(

32

)S2

2 = 88

(S2 = 2, S3 = 5)

30

Exhibit 6

1. Semantical equality of two iterates in same column connected by l impliessemantical equality of two iterates of order 2 if V satisfies unicity conditions.

A3

1 2l3 4

l2 5

A4

1 2 3 4 5l l6 7 8 9 10

l l3 4 11 12 13

l2 5 7 10 14

A5

1 2 3 4 5 6 7 8 9 10 11 12 13 14l l l l l15 16 17 18 19 20 21 22 23 224 25 26 27 28

l l l l l6 7 8 9 10 29 30 31 32 33 34 35 36 37

l l l l l3 4 11 12 13 17 18 25 26 27 38 39 40 41

l l l l l2 5 7 10 14 16 19 21 24 28 30 33 37 42

2. Semantic equality of two iterates in same column or different columns havinga common element connected by l implies semantic equality of two iterates of

order 3 if V satisfies unicity conditions.

A4

1 2 3 4 5l l6 7 8 9 10l l l l3 4 11 12 13

l l2 5 7 10 14

A5

1 2 3 4 5 6 7 8 9 10 11 12 13 14l l l l15 16 17 18 19 20 21 22 23 24 25 26 27 28l l l l l l l l6 7 8 9 10 29 30 31 32 33 34 35 36 37

l l l l l l l l3 4 11 12 13 17 18 25 26 27 38 39 40 41

l l l l2 5 7 10 14 16 19 21 24 28 30 33 37 42

31